{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:OADGQCJ2X5GCESL2KKERKR7VCG","short_pith_number":"pith:OADGQCJ2","schema_version":"1.0","canonical_sha256":"700668093abf4c22497a52891547f511843dce5299e6577cd85386c84569f2cc","source":{"kind":"arxiv","id":"0907.1450","version":2},"attestation_state":"computed","paper":{"title":"Effective Polyakov Loop Dynamics for Finite Temperature G(2) Gluodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-th"],"primary_cat":"hep-lat","authors_text":"Andreas Wipf, Bjoern H. Wellegehausen, Christian Wozar","submitted_at":"2009-07-09T19:59:41Z","abstract_excerpt":"Based on the strong coupling expansion we obtain effective 3-dimensional models for the Polyakov loop in finite-temperature G_2 gluodynamics. The Svetitsky-Jaffe conjecture relates the resulting continuous spin models with G_2 gluodynamics near phase transition points. In the present work we analyse the effective theory in leading order with the help of a generalised mean field approximation and with detailed Monte-Carlo simulations. In addition we derive a Potts-type discrete spin model by restricting the characters of the Polyakov loops to the three extremal points of the fundamental domain "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"0907.1450","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-07-09T19:59:41Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"title_canon_sha256":"15deb97a007bfe5779ec00e85946c5481dd67a8377c435df7fba5e0bd5d3c83b","abstract_canon_sha256":"5d6c5399ed55422099579143e92cc0602eefb20ce0d128c909a05acdd4dc3da9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:55.189452Z","signature_b64":"6vtrNJW3j0l+tpeMpTlCMlT+2xrdEDB+85ZhZxNRerYlON3JGFPvAuPqr4fJ84T+vUNHzI6Y4n32yf+QoWsRAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"700668093abf4c22497a52891547f511843dce5299e6577cd85386c84569f2cc","last_reissued_at":"2026-05-18T02:24:55.188705Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:55.188705Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Polyakov Loop Dynamics for Finite Temperature G(2) Gluodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-th"],"primary_cat":"hep-lat","authors_text":"Andreas Wipf, Bjoern H. Wellegehausen, Christian Wozar","submitted_at":"2009-07-09T19:59:41Z","abstract_excerpt":"Based on the strong coupling expansion we obtain effective 3-dimensional models for the Polyakov loop in finite-temperature G_2 gluodynamics. The Svetitsky-Jaffe conjecture relates the resulting continuous spin models with G_2 gluodynamics near phase transition points. In the present work we analyse the effective theory in leading order with the help of a generalised mean field approximation and with detailed Monte-Carlo simulations. In addition we derive a Potts-type discrete spin model by restricting the characters of the Polyakov loops to the three extremal points of the fundamental domain "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0907.1450","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"0907.1450","created_at":"2026-05-18T02:24:55.188828+00:00"},{"alias_kind":"arxiv_version","alias_value":"0907.1450v2","created_at":"2026-05-18T02:24:55.188828+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0907.1450","created_at":"2026-05-18T02:24:55.188828+00:00"},{"alias_kind":"pith_short_12","alias_value":"OADGQCJ2X5GC","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"OADGQCJ2X5GCESL2","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"OADGQCJ2","created_at":"2026-05-18T12:26:01.383474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG","json":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG.json","graph_json":"https://pith.science/api/pith-number/OADGQCJ2X5GCESL2KKERKR7VCG/graph.json","events_json":"https://pith.science/api/pith-number/OADGQCJ2X5GCESL2KKERKR7VCG/events.json","paper":"https://pith.science/paper/OADGQCJ2"},"agent_actions":{"view_html":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG","download_json":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG.json","view_paper":"https://pith.science/paper/OADGQCJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0907.1450&json=true","fetch_graph":"https://pith.science/api/pith-number/OADGQCJ2X5GCESL2KKERKR7VCG/graph.json","fetch_events":"https://pith.science/api/pith-number/OADGQCJ2X5GCESL2KKERKR7VCG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG/action/storage_attestation","attest_author":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG/action/author_attestation","sign_citation":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG/action/citation_signature","submit_replication":"https://pith.science/pith/OADGQCJ2X5GCESL2KKERKR7VCG/action/replication_record"}},"created_at":"2026-05-18T02:24:55.188828+00:00","updated_at":"2026-05-18T02:24:55.188828+00:00"}